Systems and methods for tracking power modulation

ABSTRACT

Apparatus and methods determine the rotational position of a spinning object. A satellite positioning system can be used to determine the spatial position of an object, which in turn can be used to guide the object. However, when the object is spinning, such as an artillery shell, then the rotational orientation should be known in order to properly actuate the control surfaces, such as fins, which will also be spinning.

CROSS-REFERENCE TO RELATED APPLICATION

This application is a continuation application of U.S. application Ser. No. 13/492,447, filed Jun. 8, 2012, now U.S. Pat. No. 8,711,035, issued on Apr. 29, 2014, which is a continuation application of U.S. application Ser. No. 13/189,962, filed Jul. 25, 2011, now U.S. Pat. No. 8,199,052, issued on Jun. 12, 2012, which is a continuation application of U.S. application Ser. No. 12/231,315, filed Aug. 29, 2008, now U.S. Pat. No. 7,986,265, issued on Jul. 26, 2011, the entireties of which are incorporated by reference herein.

BACKGROUND

1. Field of the Invention

The invention generally relates to electronics. In particular, the invention relates to a receiver for a satellite navigation system, such as the NAVSTAR Global Positioning System (GPS).

2. Description of the Related Art

A Global Positioning System (GPS) satellite radiates a spread spectrum, pseudorandom noise (PN) signal indicating the satellite's position and time. A GPS receiver that receives signals from a plurality of satellites can compute the distance to each satellite and then calculate the receiver's spatial position, spatial velocity, and time.

GPS receivers can be used in a broad variety of environments. One application is to provide spatial position and spatial velocity for a projectile, such as an artillery shell. This information can then be used by a guidance system of the projectile to guide the projectile to its intended destination.

Flight corrections can be made by manipulating fins on the projectile. However, the projectile can be configured to spin along an axis in its line of flight to stabilize flight. This spin affects the flight controls for guidance, as the fins will spin with the projectile. In order to make proper flight corrections, the rotational orientation of the projectile should be known.

SUMMARY

Apparatus and methods determine the rotational position of an object. A satellite positioning system can be used to determine the spatial position of an object, which in turn can be used to guide the object. However, for guidance of an object that spins during flight, such as an artillery shell, then the rotational orientation should also be known in order to properly time the actuation of the control surfaces. Disclosed techniques ascertain the rotational position from the satellite positioning system signals. The disclosed techniques can be used with the coarse/acquisition C/A code, precise P(Y) code, or both the C/A code and the P(Y) code.

BRIEF DESCRIPTION OF THE DRAWINGS

These drawings the associated description herein are provided to illustrate specific embodiments of the invention and are not intended to be limiting.

FIG. 1 is a schematic diagram drawn looking down the nose of a projectile and illustrates timing references and nomenclature used for the projectile and space vehicles (SVs).

FIG. 2 illustrates a top-level block diagram of a GPS launch system and a GPS projectile system according to an embodiment of the invention.

FIG. 3 illustrates one embodiment of a GPS receiver for determining the next time that the antenna will be facing up t_up.

FIG. 4 illustrates an embodiment of a SV power modulation tracking filter according to an embodiment of the invention.

FIG. 5 illustrates a phase rotator/mixer.

FIG. 6 illustrates an embodiment of a frequency-locked loop (FLL) acquisition loop.

FIG. 7 illustrates an embodiment of a 4th order phase-locked loop (PLL) SV modulation tracking loop.

FIG. 8 illustrates a process showing state transitions for GPS-based “up” estimation.

FIG. 9 illustrates an aspect angle α_(u).

FIG. 10 illustrates an azimuth angle az_(u).

DETAILED DESCRIPTION OF SPECIFIC EMBODIMENTS

Although particular embodiments are described herein, other embodiments of the invention, including embodiments that do not provide all of the benefits and features set forth herein, will be apparent to those of ordinary skill in the art.

While illustrated in the context of the NAVSTAR Global Positioning System (GPS), the principles and advantages described herein are applicable to other positioning systems, such as, but not limited to, the Russian GLONASS system, the European Galileo system, the Chinese COMPASS system, the Indian IRNSS system, or the like.

FIG. 1 is a schematic diagram drawn looking down the nose of a projectile 102 and illustrating timing references and nomenclature used for the projectile 102 and space vehicles (SVs). FIG. 1 depicts how SVs in view are used in combination to estimate the projectile's roll.

FIG. 1 illustrates the projectile 102 in the center of the diagram, one or more antennas 104, and one or more fins 106. The illustrated techniques can assess when an antenna 104 of the projectile 102 is effectively pointing to a space vehicle.

In the diagram, the projectile 102 is shown rotating counter-clockwise; however, the techniques disclosed herein are applicable to rotation in either direction. The direction of the rotation will follow the rifling of a barrel of a cannon and is typically known before the projectile is launched from the cannon.

Typically, the space vehicles sv₁, sv₂, sv₃, and sv₄, are the sources for GPS signals. However, other sources, such as beacons, can be applicable. The number of space vehicles used by the projectile 102 can vary in a broad range, but typically reception to at least four space vehicles is needed to resolve spatial position.

The receiver for the projectile 102 has a plurality of phase-locked loops (PLLs) for determining the angular orientation of SVs based on signal power modulation. In the illustrated embodiment, for each SV, there is a corresponding PLL of the receiver for determining when the antenna pattern of the antenna 104 is generally pointing towards a particular SV, referred to as “up.” This “pointing towards” refers to the rotation and not to an aspect angle. In the illustrated embodiment, these PLLs along with line-of-sight (LOS) vector information are used to calculate the time (t_up_(i)) when the pattern of the antenna 104 will be pointing “up” with respect to a particular i-th SV. In one embodiment, this “next up time” t_up_(i) is independently calculated for each SV in view of the receiver, and then the independent calculations are averaged together, which averages out errors.

This averaged “next up time” is represented by variable t_up. At the averaged next up time t_up, the pattern of the antenna 104 of the projectile 102 is “pointing” at the average of the independent up times, so that the average is generally pointing away from the center of the earth. The averaged next up time t_up is provided as an index for flight control.

A next up time t_up_(i) for a particular i-th space vehicle SV_(i) represents a time estimate of the next time that the pattern of the antenna 104 faces towards the i-th space vehicle SV_(i). Every space vehicle in view can be used to estimate a particular next up time t_up_(i), but an individual estimate is relatively noisy due to the stochastic nature of a phase-locked loop. Averaging multiple up time estimates t_up_(i) smoothes this noise and provides a more accurate estimate for a reference time t_up when the pattern of the antenna will be in a particular orientation, in this case, up with respect to an average. In the illustrated embodiment, equal weighting is used for the averaging; however, an unequally weighted average can also be used. For example, signals received from space vehicles with lower signal power can be weighted less heavily than signals received from space vehicles with higher signal power.

FIG. 2 illustrates a top-level block diagram of a launch system 202 and a projectile system 204 according to an embodiment of the invention. FIG. 2 illustrates electronic components for the launch system 202. Other components can include, for example, a cannon for the launch of a projectile. The launch system 202 components are typically reusable, and are used, for example, on the ground, in a truck, in a ship, in an airplane, or the like. The launch system 202 includes a base station GPS receiver 206 and a destination/flight path selector 208.

The base station GPS receiver 206 receives GPS signals and communicates information to the projectile system 204 such that the projectile system 204 can readily acquire the GPS signals after launch. In a GPS receiver, “acquiring” a satellite occurs when the GPS receiver acquires the signal of a satellite. The GPS receiver acquires the satellite by matching a code received by the GPS receiver to a code defined for the satellite. In an enhancement, the matching is performed to the carrier wave that is carrying the ranging code. This code and/or carrier phase matching is termed “correlation.” For example, when the projectile system 204 is loaded into a cannon for launch, it is typically not able to receive normal GPS signals. Accordingly, the base station GPS receiver 206 can preload a GPS receiver 210 with data indicating which satellites are in the area for reception, GPS system time, ephemeris data for the satellites, and the like. The destination/flight path selector 208 provides information such as a flight path to an intended destination for the projectile. In one embodiment, an interface such as an inductive coupler is used to preload the GPS data and the intended flight path data from the launch system 202 to the projectile system 204 before the projectile is launched. After the projectile is launched, the launch system 202 and the projectile system 204 are typically not in communication. The intended flight path data can also include expected velocity at various points along the intended flight path. Of course, other data can also be provided, and status communication can also be returned from the projectile system 204 to the launch system 202.

The projectile system 204 includes the GPS receiver 210, a guidance computer 212, and a flight control 214. For clarity, other components of the projectile system 204, such as the components of an artillery shell, are not shown. For example, the flight control 214 can correspond to actuators for moving or deforming fins, to brakes, or the like. These actuators can be electromechanical, piezoelectric, or the like. An input sgn(r′), which can be provided by the launch system 202, indicates rotational direction of the projectile during flight.

In the illustrated embodiment, the GPS receiver 210 and the guidance computer 212 both receive the intended flight path. In the illustrated embodiment, line-of-sight (LOS) vectors are calculated using the intended flight path and time. The LOS vectors will be described in greater detail later in connection with FIG. 3. In an alternative embodiment, the LOS vectors are computed conventionally, that is, using the position of the projectile as obtained via GPS and the position of the satellites.

The GPS receiver 210 provides the spatial position of the projectile to the guidance computer 212 so that the guidance computer 212 can make adjustments to the actual flight path. Such adjustments can be one-dimensional (range only) as encountered with brakes, or can be two-dimensional.

The GPS receiver 210 also provides the guidance computer 212 with a reference time to indicate rotation. In the illustrated embodiment, the reference time t_up is referenced to GPS system time, and indicates when the projectile is expected to be “up,” that is, would have a particular angular position. The particular angular position can be used as an index by the guidance computer 212. In the illustrated embodiment, the particular angular position is the average of “up” positions to the satellites in view. While this average can vary over time, it is fixed enough to be useful for guidance. In an alternate embodiment, the GPS receiver 210 can provide a different type of indicator, such as, for example, an edge on a clock signal, a data register indicating approximate angle, or the like. One embodiment of the GPS receiver 210 will be described in greater detail later in connection with FIG. 3.

As described earlier, both the GPS receiver 210 and the guidance computer 212 receive the intended flight path. The guidance computer 212 also receives the spatial position from the GPS receiver 210 and determines whether or not to adjust the actual flight path. If the projectile is spinning and is guided by manipulating fins, then the fins will typically be spinning with the projectile. The guidance computer 212 uses the rotation indicator sgn(r′) to determine how to actuate the flight controls to adjust the actual flight path.

FIG. 3 illustrates a system diagram for one embodiment of the GPS receiver 210 for estimating an averaged next up time t_up. Initialization data 302, such as data coupled from the launch system 202 (FIG. 2), can include space vehicle ephemeris data, GPS system time, both as determined by the base station GPS receiver 206, and an intended trajectory or nominal trajectory for the projectile. A dashed line separates components for a positioning processor 350 and components for a roll processor 360. In the illustrated embodiment, the positioning processor 350 portion of the GPS receiver 210 is conventional.

Various components can be implemented in hardware, in software/firmware, or in a combination of both hardware and software/firmware. In one embodiment, the hardware correlators 310 and the code/carrier numerically controlled oscillators 316 are implemented by hardware, and the other components of the GPS receiver 210 are implemented in software/firmware. For example, executable instructions can be stored in a computer-readable medium, such as RAM or ROM memory, and executed by a processor, such as a microprocessor. For example, the instructions can be embedded into flash ROM of the GPS receiver 210. In another example, the instructions can be loaded into RAM from the launch system 202.

In the illustrated embodiment, after initialization from the launch system 202, an independent timer 304 maintains a “current time,” which is denoted with variable t_(curr). The current time t_(curr) is independent of GPS signals received by the GPS receiver 210 and independent of GPS system time after launch. In one embodiment, the timer 304 is maintained by software/firmware.

In the illustrated embodiment, the positioning processor 350 is conventional. For example, the illustrated positioning processor 350 includes hardware correlators 310, a deep integration filter 312, a navigation Kalman filter 314, and code/carrier numerically controlled oscillators 316 arranged in a tracking loop. Received GPS signals are provided as an input to the HW correlators 310. The HW correlators 310 correlate the received GPS signal with the receiver's best estimate of a replica signal to generate in-phase (I) and quadrature-phase data (Q) that contain projectile position error measurements and SV power measurements. In one embodiment, the navigation Kalman filter 314 has 12 states and computes position, velocity, acceleration, and time. For clarity, antennas and front-end components of the GPS receiver 210 are not shown in FIG. 3. An output of the positioning processor 350 is the ECEF position, velocity, and time, which is provided as an input to the guidance computer 212.

In the illustrated embodiment, for calculating LOS vectors, an LOS estimator 306 estimates its location using the current time t_(curr) and the intended or nominal trajectory (preloaded), and estimates the location of a space vehicle using the current time t_(curr) and the SV ephemeris data (preloaded). The LOS estimator 306 can be implemented in hardware or in software/firmware. In the illustrated embodiment, the LOS estimator 306 is implemented in software/firmware. Advantageously, the LOS vectors can be computed even when the GPS receiver 210 encounters interference. This can improve tracking under certain circumstances and reduce computation time in flight.

In FIG. 3, subscript n indicates a particular navigation channel, subscript u indicates a particular upfinder channel, subscript c indicates the set of all channels, Δφ_(u) indicates phase compensation. LOS data can include, for example, the aspect angle α_(u) to a u-th space vehicle (see, for example, FIG. 9, SVs projected on the vertical plane through the longitudinal axis of the projectile 102), and the azimuth angle az_(u) in an up-starboard plane to the u-th upfinder source (see, for example, FIG. 10, SVs projected on a horizontal plane). As illustrated in FIG. 9, the aspect angle α_(u) is between the longitudinal axis of the u-th space vehicle SV_(u) (projected rearward to the projectile 102) and the line of sight to the projectile 102 measured from the tail of the u-th space vehicle SV_(u).

The I and Q data for the positioning processor 350 (subscript n) or for the roll processor 360 (subscript u) corresponds to a correlated in-phase output and a quadrature-phase of the HW correlators 310. In one embodiment, the roll processor 360 is entirely implemented in software/firmware, but can also be implemented in hardware. In the illustrated embodiment, the roll processor 360 tracks each SV in view using a phase-locked loop for each SV, but typically uses less than all the trackable SVs to compute the aggregate up time t_up as will be discussed in greater detail in the following.

A SV power modulation tracking filter 320 incorporates both a frequency-locked loop (FLL) and a phase-locked loop (PLL). A mode/state_(u) status indicates whether the SV power modulation tracking filter 320 is operating in FLL mode or in PLL mode, and whether or not the loop is locked (for the u-th SV). The mode/state_(u) information is provided as an input to a measurement enabler 328. Further details of the SV power modulation tracking filter 320 will be described later in connection with FIG. 4. In one embodiment, the SV power modulation tracking filter 320 is implemented by software/firmware. Preferably, each SV in view is tracked by the SV power modulation tracking filter 320.

The SV power modulation tracking filter 320 isolates the power modulation on the I/Q data that is a result of the projectile's spin. The SV power modulation tracking filter 320 phase locks to the amplitude modulation of the GPS signal caused by the projectile's spin. This phase information (angle) is then combined with LOS information from the LOS estimator 306. In the illustrated embodiment, the combination of the phase information and the LOS information is performed in a projectile antenna up estimator 324. In the illustrated embodiment, the LOS information is derived from the position, velocity, and time (PVT) information based on preloaded information from the timer 304 and the initialization data 302, that is, information that is not obtained from GPS signals by the positioning processor 350 during the flight of the projectile 102.

The line-of-sight (LOS) vectors from the LOS estimator 306 are provided as an input to the navigation Kalman filter 314 and to the projectile antenna up estimator 324. In the illustrated embodiment, the LOS vectors used by the navigation Kalman filter 314 are based only on preloaded initialization data 302 (ephemeris and trajectory) and on the time maintained by the timer 304. However, in an alternative embodiment, the LOS vectors can also be computed in a conventional manner.

Aspect angles α_(u) are provided as an input to the roll compensator 322 and to the measurement enabler 328. The roll compensator 322 is optional. Azimuth angles az_(u) are provided as an input to the projectile antenna up estimator 324. In an alternative embodiment, the LOS vectors are computed in another manner, such as the conventional practice of determining the position of the GPS receiver 210 via GPS signal tracking and determining the position of a space vehicle from received ephemeris data.

As the projectile 102 (FIG. 1) spins during flight, the pattern of the antenna 104 (FIG. 1) will at times point toward a SV and at times away from the SV. This rotation induces a power modulation on the received GPS signal that is detectable as an amplitude modulation having a modulation rate (frequency) that is the same as the spin of the projectile 102. In the illustrated embodiment, the SV power modulation tracking filter 320 only phase locks to the amplitude modulation (due to rotation) of a GPS signal from a SV and does not monitor phase modulation (due to rotation). Typically, the lobes of the antenna 104 point outwards from the projectile 102. Preferably, the antenna 104 is configured such that its main lobe points normal to the flight trajectory; however, it will be understood that depending on the angle that a particular SV has with respect to the projectile 102, it may not be the main lobe that has the strongest overall power. In addition, it should be noted that it can be difficult to detect the amplitude modulation of the GPS signal when a SV is too far in the direction of the nose or the tail of the projectile 102, for example, directly in front of or behind the projectile 102. In one embodiment, SVs that make an angle within 45 degrees of the nose or 50 degrees from the tail are not used for up determination, that is, are not part of the “u” set of SVs, and an up time t_up_(u) for those SVs is not computed. However, these SVs may still be used for obtaining positioning information, that is, may be used as one of the “n” set of SVs.

The roll compensator 322 receives the aspect angle α_(u) as an input, and generates phase compensation Δφ_(u) as an output. The phase compensation Δφ_(u) provides a correction factor used by the projectile antenna up estimator 324 to compensate for the antenna pattern. In one embodiment, the roll compensator 322 is implemented with a lookup table (LUT). In one embodiment, the roll compensator 322 is optional. For example, if the antenna pattern gain and phase is relatively symmetric over +/−180 degrees, then the roll compensator 322 can be omitted. In one embodiment, the roll compensator 302 further receives an estimate of the expected roll rate (not shown) from the initialization data 302 and the computed roll rate φ′_(u) from the SV power modulation tracking filter 320 as a check of the computed roll rate φ′_(u). The expected roll rate typically varies over the intended trajectory. If the expected roll rate and the computed roll rate φ′_(u) do not agree to within a threshold, then the computed roll rate φ′_(u) can be determined to be untrustworthy, and the roll and roll rate estimate for the particular SV can be discarded as invalid. For example, the threshold can be predetermined, such as a threshold of +/−20 Hz.

In one embodiment, the projectile antenna up estimator 324 is a Kalman filter. The Kalman filter smoothes the up estimate for each SV tracked. The projectile antenna up estimator 324 uses the amplitude modulation information from the SV power modulation tracking filter 320, the direction of the spin sgn(r′) (either 1 or −1), and the phase compensation Δφ_(u) to generate an estimate of the u-th SV's angular position, angular velocity, and angular acceleration relative to the projectile 102. This information is summarized in vector x. In one embodiment, the projectile antenna up estimator 324 is implemented in software/firmware. In the illustrated embodiment, the projectile antenna up estimator 324 performs the computations expressed in Equations 1 and 2. Equation 1 describes a roll estimate vector x describing rotation with respect to a particular u-th SV. The components of the roll estimate vector x include phase or angle r, angular velocity r′, and angular acceleration r″. In the illustrated embodiment, the phase or angle r is referenced to the particular u-th SV, with 0 angle being with the antenna 104 (FIG. 1) pointing towards the u-th SV,

$\begin{matrix} {x = {\begin{bmatrix} r \\ r^{\prime} \\ r^{''} \end{bmatrix}_{u} = \begin{bmatrix} {{az} - {\left( {\varphi + {\Delta\varphi}} \right){{sgn}\left( r^{\prime} \right)}}} \\ {\varphi^{\prime}{{sgn}\left( r^{\prime} \right)}} \\ {\varphi^{''}{{sgn}\left( r^{\prime} \right)}} \end{bmatrix}_{u}}} & \left( {{Eq}.\mspace{14mu} 1} \right) \end{matrix}$

Equation 2 illustrates a covariance matrix R for a Kalman filter for the noise estimated by the FLL/PLLs.

$\begin{matrix} {R_{u} = \begin{bmatrix} \sigma_{\varphi}^{2} & 0 & 0 \\ 0 & \sigma_{\varphi^{\prime}}^{2} & 0 \\ 0 & 0 & \sigma_{\varphi^{''}}^{2} \end{bmatrix}_{u}} & \left( {{Eq}.\mspace{14mu} 2} \right) \end{matrix}$

The measurement enabler 328 controls a measurement window 326 for monitoring the roll estimate vector x output of the projectile antenna up estimator 324. In the illustrated embodiment, the measurement window 326 is open for a measurement associated with a u-th SV when the following conditions are true: (a) the SV power modulation tracking filter 320 is in PLL mode; (b) the PLL is locked; and (c) aspect angle az_(u) to the u-th SV is between 45 degrees and 135 degrees. Other applicable aspect angles will be readily determined by one of ordinary skill in the art and can depend on the antenna pattern. Beyond the selected range for the aspect angle az_(u), the amount of amplitude modulation caused by the spinning of the projectile 102 is deemed to be relatively small. Thus, while the SV power modulation tracking filter 320 preferably tracks all the SVs in view, the operation of the measurement window 326 limits the SVs used to generate the aggregate up time t_up to a smaller subset. The SVs in the smaller subset can change over time as the projectile 102 travels and its aspect angle changes. The measurement window 326 can be embodied in software/firmware by, for example, inspecting a limited range of data.

A current roll estimate generator 330 generates a current roll estimate vector x_(curr) based on the current time t_(curr), the roll estimate vector x, and a previous up time t_(u), that is, when the antenna 104 was last pointing at the u-th SV. The foregoing data is combined with a transition matrix Φ (see Eq. 3). The current roll estimate vector x_(curr) has the same dimensions as the roll estimate vector x of Equation 1. The current roll estimate vector x_(curr) can include an estimate of the angle r, angular velocity r′, and optionally an angular acceleration r″ of the antenna 104 relative to the SV for the current time t_(curr). In one embodiment, the current roll estimate generator 330 is embodied by software/firmware.

$\begin{matrix} {\Phi = \begin{bmatrix} 1 & {\Delta \; t} & {\frac{1}{2}\Delta \; t^{2}} \\ 0 & 1 & {\Delta \; t} \\ 0 & 0 & 1 \end{bmatrix}} & \left( {{Eq}.\mspace{14mu} 3} \right) \end{matrix}$

The next up time estimator 332 determines an estimate (in time) of the next time that the pattern of the antenna 104 will be pointing toward the u-th SV. The information can be computed as illustrated within next up time estimator 332 based on the current time t_(curr) and the angle (r) and the angular velocity (r′) of the current information vector x_(curr). A particular up time output of next up time estimator 332 corresponds to the next up time t_up_(u) for the u-th upfinder channel.

The various next up times t_up_(u) are then aggregated to form the next up time t_up for the projectile 102 as a whole. For example, as discussed earlier in connection with FIG. 1, the aggregated next up time t_up can be formed by calculating an average of the next up times from the set of up times for the u SVs.

FIG. 4 illustrates an embodiment of the SV power modulation tracking filter 320 according to an embodiment of the invention. The SV power modulation tracking filter 320 includes a phase rotator/mixer 402, a frequency-locked loop (FLL) acquisition loop 404, a 4th-order phase-locked loop (PLL) tracking loop 406, an FLL lock detector 408, a mode selector 410, and a phase lock detector 412. There should be a separate SV power modulation tracking filter 320 for each SV that is tracked. In one embodiment, there are at least 12 separate SV power modulation tracking filters 320. When implemented in software/firmware, the same routine can be used for each SV that is tracked. When implemented in hardware, preferably, each of the SV power modulation tracking filters 320 is identical to each other. However, when implemented in hardware, some components, such as the FLL acquisition loop 404, the FLL lock detector 408 or selected components thereof, can be shared among two or more SV power modulation tracking filters 320. For example, after phase locking by the PLL tracking loop 406, the FLL components are typically not used in operation, and can be used for acquisition to a different SV. In addition, the roll frequency of the projectile 102 is caused by the rolling of the projectile 102 itself, and thus, the power modulation should have the same frequency (the roll frequency) among the various SVs. Thus, a FLL acquisition loop 404 for one SV can be used for pulling in a PLL tracking loop 406 for another. When implemented in software/firmware, the routine implementing the FLL would not need to be called after the PLL tracking loop 406 is locked.

In the illustrated embodiment, outputs of the 4th-order PLL tracking loop 406 include roll phase φ_(u), roll rate φ′_(u), roll acceleration φ″_(u), which are available from the loop filter 704 (FIG. 7). In one embodiment, standard deviations of each are also computed and depicted as σ_(φu), σ_(φ′u), σ_(φ″u).

One embodiment of the phase rotator/mixer 402 will be described in greater detail later in connection with FIG. 5. One embodiment of the frequency-locked loop (FLL) acquisition loop 404 will be described in greater detail later in connection with FIG. 6. One embodiment of the 4th-order phase-locked loop (PLL) tracking loop 406 will be described in greater detail later in connection with FIG. 7.

The phase rotator/mixer 402 utilizes mixers to phase rotate the input I_(CORR) and Q_(CORR) to generate I_(ROT) and Q_(ROT) as outputs. The I_(CORR) and the Q_(CORR) signals correspond to the particular I_(U) and Q_(U) signals for the u-th SV. The phase rotation is controlled by the roll phase estimate. The FLL acquisition loop 404 determines the roll rate (frequency) to assist the PLL tracking loop 406 to pull in to achieve phase lock. After the PLL tracking loop 406 achieves phase lock, then the PLL tracking loop 406 is used to track the roll of the projectile 102. The FLL lock detector 408 is used for acquisition of the signal modulation and generates a roll rate error (frequency). Based on the roll rate error from the FLL lock detector 408 and the pull-in range of the PLL tracking loop 406, the mode selector 410 selects between the FLL acquisition loop 404 or the PLL tracking loop 406. The phase lock detector 412 determines whether or not PLL tracking loop 406 is phase locked.

FIG. 5 illustrates one embodiment of the phase rotator/mixer 402. In the illustrated embodiment, the phase rotator/mixer 402 is embodied in software/firmware. However, the phase rotator/mixer 402 can alternatively be embodied in hardware. The spin of the projectile 102 causes a power modulation on the received GPS signals. When the main lobe of the antenna (assuming a symmetrical antenna pattern) of the projectile 102 faces a particular SV, then maximum power for the received GPS signal is received. When the antenna faces away from the SV, minimum power is received. This power modulation is similar to a sine wave over time, and the PLL tracking loop 406 tracks the phase of that amplitude modulated pattern.

The phase rotator/mixer 402 includes a magnituder 502, a magnitude lossy integrator 504, a summer 506, a sine function block 508, a cosine function block 510, an I-phase mixer 512, a Q-phase mixer 514, an I-phase lossy integrator 516, a Q-phase lossy integrator 518.

The magnituder 502 generates a raw magnitude signal that has the magnitude of the I_(CORR) and Q_(CORR) signals. The magnitude lossy integrator 504 is a low-pass filter. In one embodiment, the time constant of the magnitude lossy integrator 504 is about 128 milliseconds. The time constant should be relatively long relative to the spin interval of the projectile 102, which is typically around 4 milliseconds, but varies within a wide range. The time constant can vary in a very broad range and other applicable time constants will be readily determined by one of ordinary skill in the art. The output of the magnitude lossy integrator 504 contains the DC component of the raw magnitude signal, and the DC component is subtracted from the raw magnitude signal by the summer 506 to generate a signal referred to as a real input signal.

A sine and cosine of a roll phase estimate are generated by the sine function block 508 and by the cosine function block 510, respectively. The sine function block 508 and the cosine function block 510 can be implemented by, for example, a lookup table or by a function call. When the SV power modulation tracking filter 320 is phase locked, the sine and cosine of the roll phase estimate are phase-locked to the reference inputs I_(CORR) and Q_(CORR). In one embodiment, the roll phase estimate is an output of the mode selector 410 (FIG. 4). The I-phase mixer 512 and to the Q-phase mixer 514 form a phase detector. The sine and cosine of the roll phase estimate are provided as inputs to the I-phase mixer 512 and to the Q-phase mixer 514, respectively, which mixes the sine and cosine with the real input signal for phase detection. The outputs of the I-phase mixer 512 and to the Q-phase mixer 514 represents a difference in phase between the reference inputs I_(CORR) and Q_(CORR) and the sine and cosine of the roll phase estimate. The outputs of the I-phase mixer 512 and the Q-phase mixer 514, respectively, are provided as inputs to the I-phase lossy integrator 516 and to the Q-phase lossy integrator 518, respectively.

The I-phase lossy integrator 516 and the Q-phase lossy integrator 518 are low-pass filters that remove sidebands from the outputs of the I-phase mixer 512 and the Q-phase mixer 514, respectively, to generate the outputs I_(ROT) and Q_(ROT) of the phase rotator/mixer 402. The I-phase lossy integrator 516 and the Q-phase lossy integrator 518 form a complex low pass filter. In the illustrated embodiment, the 2-sided bandwidth (2BW) point is 100 Hertz (50 Hz each). Other applicable bandwidth specifications are applicable and will be readily determined by one of ordinary skill in the art. However, it should be noted that the 2-sided bandwidth for the complex low-pass filter formed by the I-phase lossy integrator 516 and the Q-phase lossy integrator 518 should be much wider than the 2-sided bandwidth for the loop.

FIG. 6 illustrates an embodiment of the FLL acquisition loop 404. The FLL acquisition loop 404 includes a phase differentiator 602, a loop filter 604, and a roll-phase integrator 606. The phase differentiator 602 generates a roll rate error as an output. The roll rate error output of the phase differentiator 602 is provided as an input to the FLL lock detector 408 (FIG. 4) and as an input to the loop filter 604. In the illustrated embodiment, the loop filter 604 has a roll acceleration integrator and a roll rate integrator. An output of the loop filter 604 is provided as an input to the roll phase integrator 606, which generates a roll phase as an output. The FLL acquisition loop 404 assists the PLL tracking loop 406 (FIG. 4) to achieve phase lock. For example, the PLL tracking loop 406 is typically unable to acquire phase lock to the reference inputs I_(CORR) and Q_(CORR) unless the frequency error or roll rate error is within a certain range, typically a few hertz for the illustrated embodiment of the PLL tracking loop 406. After the PLL tracking loop 406 is locked, the operation of the FLL acquisition loop 404 is typically not needed.

The FLL lock detector 408 (FIG. 4) senses when the roll rate error is within the pull-in range of the PLL tracking loop 406. In one embodiment, the FLL lock detector 408 is configured to receive the roll rate error as an input to a lossy integrator to generate a filtered roll rate error, to take the absolute value of the integrated roll rate error, to compare the integrated roll rate error to a threshold, such as a few hertz, and then to determine that the FLL acquisition loop 404 is locked if the roll rate is below the threshold and unlocked if otherwise. The state of locked/unlocked can be used to determine whether or not the roll rate error is within the pull-in range of the PLL tracking loop 406.

FIG. 7 illustrates an embodiment of the PLL tracking loop 406 implemented as a 4-th order PLL tracking loop. The PLL tracking loop 406 has a phase detector 702, a loop filter 704, and a roll-phase integrator 706. A roll phase error output of the phase detector 702 is provided as an input to the loop filter 704. A roll rate output of the loop filter 704 is provided as an input to the roll-phase integrator 706, which generates a roll phase output in cycles. The phase lock detector 412 (FIG. 4) detects when the PLL tracking loop 406 is phase locked to the reference inputs I_(CORR) and Q_(CORR).

In one embodiment, the phase lock detector 412 is configured to low-pass filter the I_(ROT) and Q_(ROT) outputs of the phase rotator/mixer 402 with lossy integrators. The bandwidth of these lossy integrators should be less than the bandwidth of the PLL tracking loop 406. While phase locked, most of the power should be in the filtered I_(ROT) signal and relatively little should be in the filtered Q_(ROT) signal. This relationship can be used to determine whether the PLL tracking loop 406 is locked. In one embodiment, the phase lock detector 412 is configured to take the absolute value of the filtered Q_(ROT) signal, and then multiply the filtered Q_(ROT) signal by a lock threshold value. In one embodiment, the lock threshold value is around 1.5. However, the lock threshold value can vary in a relatively broad range and other applicable values will be readily determined by one of ordinary skill in the art. The multiplied and filtered Q_(ROT) signal is then compared with the filtered I_(ROT) signal. In one embodiment, if the multiplied and filtered Q_(ROT) signal is less than the filtered I_(ROT) signal, then the phase lock detector 412 determines that the PLL tracking loop 406 is locked. Otherwise, the phase lock detector 412 determines that the PLL tracking loop 406 is unlocked. The status mode/state_(u) can be provided as an input to the measurement enabler 328.

FIG. 8 illustrates a process showing state transitions for GPS-based “up” estimation for control of the FLL acquisition loop 404 and PLL tracking loop 406. The illustrated process can be used with either a software/firmware implementation or a hardware implementation. In the illustrated embodiment, software/firmware is used.

The process begins in an idle state 802. When commanded to track the rotation relative to a previously untracked SV, the process proceeds to an acquisition state 804 to phase lock to the SV. The process begins by closing the feedback loop of the SV power modulation tracking filter 320 (FIG. 3) around the FLL acquisition loop 404 (FIG. 4). The process stays in the acquisition state 804 until the frequency error is within the pull-in range of the PLL tracking loop 406 (FIG. 4).

When the frequency error is within the pull-in range of the PLL tracking loop 406, the process advances to a phase state 806, in which the PLL tracking loop 406 phase locks to the spin modulation on the signal from the SV. The process stays in the phase state 806 unless a new SV is commanded to be tracked, in which case, the process returns from the phase state 806 to the idle state 802, or if a loss of phase lock is detected, in which case, the process returns from the phase state 806 to the acquisition state 804.

Various embodiments have been described above. Although described with reference to these specific embodiments, the descriptions are intended to be illustrative and are not intended to be limiting. Various modifications and applications may occur to those skilled in the art. 

1. (canceled)
 2. An apparatus comprising: a projectile antenna up estimator configured to: receive at least a roll phase and roll rate of an amplitude modulation of a signal from a first space vehicle, wherein the amplitude modulation is caused by spinning of a projectile; receive an azimuth angle associated with the first space vehicle; and determine a first state of a spin of the projectile for a first time based at least partly on the roll phase, roll rate, and the azimuth angle.
 3. The apparatus of claim 2, wherein the projectile antenna up estimator is further configured to receive a roll acceleration of the amplitude modulation of the signal from the first space vehicle, wherein the first state of the spin is further determined based on the roll acceleration.
 4. The apparatus of claim 2, further comprising a next up time estimator configured to estimate a future time when the antenna of the projectile will be pointing up based on information derived from the first state.
 5. The apparatus of claim 2, further comprising a current roll estimate generator configured to: extrapolate a second state of the projectile for a second time based on the first state and the first time; and estimate a third time when the antenna of the projectile will be pointing up based at least partly on the second state.
 6. The apparatus of claim 2, wherein the projectile antenna up estimator is further configured to: receive roll phase and roll rate of an amplitude modulation of a plurality of signals from a plurality of space vehicle, wherein the amplitude modulation is caused by spinning of the projectile; receive azimuth angles associated with the plurality of space vehicles; determine a first plurality of states of the spin of the projectile based at least partly on the roll phase, roll rate, and the azimuth angle for each of the plurality of signals; estimate a plurality of future times when the antenna of the projectile will be pointing up; and combine at least a portion of the plurality of future times to generate an index for flight control.
 7. The apparatus of claim 6, wherein the projectile antenna up estimator is further configured to: receive roll acceleration of the amplitude modulation for the plurality of signals from the plurality of space vehicles, wherein the first plurality of states of the spin are further determined based on the roll acceleration for each of the plurality of signals.
 8. The apparatus of claim 6, wherein the projectile antenna up estimator is further configured to combine the at least portion of the plurality of future times by averaging.
 9. The apparatus of claim 6, further comprising a current roll estimate generator configured to extrapolate a second plurality of states of the projectile for a current time based on the first plurality of states, wherein the plurality of future times are estimated based at least partly on the second plurality of states.
 10. The apparatus of claim 6, further comprising a measurement window configured to filter out measurements such that the at least portion of the plurality of future times that are combined correspond to the future times corresponding to signals received with an azimuth angle between 45 degrees and 135 degrees.
 11. The apparatus of claim 6, wherein the projectile antenna up estimator comprises a Kalman filter.
 12. A method of generating spin information for flight control of a projectile, the method comprising: receiving at least a roll phase and roll rate of an amplitude modulation of a signal from a first space vehicle, wherein the amplitude modulation is caused by spinning of a projectile; receiving an azimuth angle associated with the first space vehicle; and determining a first state of a spin of the projectile for a first time based at least partly on the roll phase, roll rate, and the azimuth angle.
 13. The method of claim 12, further comprising: receiving a roll acceleration of the amplitude modulation of the signal from the first space vehicle; wherein the first state of the spin is further determined based on the roll acceleration.
 14. The method of claim 12, further comprising estimating a future time when the antenna of the projectile will be pointing up based on information derived from the first state.
 15. The method of claim 12, further comprising: extrapolating a second state of the projectile for a second time based on the first state and the first time; and estimating a third time when the antenna of the projectile will be pointing up based at least partly on the second state.
 16. The method of claim 12, further comprising: receiving roll phase and roll rate of an amplitude modulation of a plurality of signals from a plurality of space vehicle, wherein the amplitude modulation is caused by spinning of the projectile; receiving azimuth angles associated with the plurality of space vehicles; determining a first plurality of states of the spin of the projectile based at least partly on the roll phase, roll rate, and the azimuth angle for each of the plurality of signals; estimating a plurality of future times when the antenna of the projectile will be pointing up; and combining at least a portion of the plurality of future times to generate an index for flight control.
 17. The method of claim 15, further comprising: receiving roll acceleration of the amplitude modulation for the plurality of signals from the plurality of space vehicles; wherein the first plurality of states of the spin are further determined based on the roll acceleration for each of the plurality of signals.
 18. The method of claim 15, wherein combining comprises averaging.
 19. The method of claim 15, further comprising: extrapolating a second plurality of states of the projectile for a current time based on the first plurality of states; wherein the plurality of future times for when the antenna of the projectile will be pointing up are estimated based at least partly on the second plurality of states.
 20. The method of claim 15, wherein the at least portion of the plurality of future times that are combined correspond to the future times corresponding to signals received with an azimuth angle between 45 degrees and 135 degrees.
 21. The method of claim 12, wherein determining comprises using a Kalman filter. 